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US4597288A - Barometer - Google Patents

Barometer Download PDF

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Publication number
US4597288A
US4597288A US06/715,496 US71549685A US4597288A US 4597288 A US4597288 A US 4597288A US 71549685 A US71549685 A US 71549685A US 4597288 A US4597288 A US 4597288A
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United States
Prior art keywords
piezoelectric oscillator
output
current
voltage
control circuit
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
US06/715,496
Inventor
Hideaki Kyogoku
Fujio Tamura
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Seiko Instruments Inc
Original Assignee
Seiko Instruments Inc
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Filing date
Publication date
Priority claimed from JP5803284A external-priority patent/JPS60201225A/en
Priority claimed from JP13067684A external-priority patent/JPS6110735A/en
Application filed by Seiko Instruments Inc filed Critical Seiko Instruments Inc
Assigned to SEIKO INSTRUMENTS & ELECTRONICS LTD. reassignment SEIKO INSTRUMENTS & ELECTRONICS LTD. ASSIGNMENT OF ASSIGNORS INTEREST. Assignors: KYOGOKU, HIDEAKI, TAMURA, FUJIO
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Publication of US4597288A publication Critical patent/US4597288A/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L9/00—Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means
    • G01L9/0001—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means
    • G01L9/0008—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations
    • G01L9/0022—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations of a piezoelectric element
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10S73/00—Measuring and testing
    • Y10S73/04—Piezoelectric

Definitions

  • This invention relates to a barometer utilizing a piezoelectric oscillator.
  • FIG. 3 An oscillator 1 generates an a.c. voltage e s of a frequency f.
  • Reference numerals 2 and 3 represent an element to be measured and an amplifier, respectively. They constitute a current-voltage converter together with a feedback resistor R F , and the output voltage of the converter is e o .
  • the amplifier is selected so that a current i x , flowing through the element to be measured, and a current i F , flowing through the feedback resistor, are equal.
  • the a.c. resistance Z x of the element to be measured is determined by the equation (1):
  • FIG. 1 is a circuit block diagram showing a barometer in accordance with the present invention
  • FIG. 2 is a diagram showing an a.c. resistance -v- pressure curve of an ordinary piezoelectric oscillator
  • FIG. 3 is a circuit diagram showing a prior art current-voltage conversion circuit
  • FIG. 4 is a diagram showing the pressure dependence of the resonant frequency of an ordinary piezoelectric oscillator
  • FIG. 5 is a diagram showing the phase of the impedance of an ordinary piezoelectric oscillator.
  • FIG. 6 is a circuit block diagram showing the barometer in accordance with another embodiment of the invention.
  • FIG. 7 is a circuit block diagram showing the barometer in accordance with another embodiment of the invention.
  • FIG. 1 is a circuit diagram showing the barometer in accordance with the present invention.
  • Reference numeral 5 represents a frequency control circuit such as a voltage control oscillator which is capable of changing said frequency.
  • the variable frequency range of this frequency control circuit 5 is wider than the shift of the resonant frequency within the pressure range to be measured by the piezoelectric oscillator 6.
  • the output from the frequency control circuit 5 is applied to the piezoelectric oscillator 6, and the output of this oscillator 6 is applied to a current-voltage converter 7.
  • the current-voltage converter 7 generates a voltage proportional to a current flowing through the piezoelectric oscillator 6.
  • phase characterstics of the a.c. resistance of the piezoelectric oscillator 6, that is, the impedance, is zero (degrees) at the resonant frequency f o as shown in FIG. 5. Therefore, the phase characteristics of the output voltage of the frequency control circuit 5 are the same as those of the output voltage of the current-voltage converter 7 at the resonant frequency f o , but the voltage of the current-voltage converter 7, having the same phase as the current flowing through the piezoelectric oscillator 6, lags behind the output voltage of the frequency control circuit 5 at frequencies lower than the resonant frequency.
  • a phase comparator 8 detects the phase difference between the output voltage of the frequency control circuit 5 and the output voltage of the current-voltage converter 7.
  • the phase comparator 8 generates a voltage proportional to the phase difference.
  • This output voltage is in turn applied to a frequency control terminal of the frequency control circuit 5, and a feedback loop is formed so that the frequency of the voltage applied to the piezoelectric oscillator 6 always coincides with the resonant frequency.
  • Reference numeral 9 represents a low-pass filter which is connected to the phase comparator 8. Normally, the low-pass filter 9 is disposed so as to eliminate the high frequency component (noise) of the output of the phase comparator 8 and to stabilize the system.
  • the output of the current-voltage converter 7 can be expressed by the following equation (2) from equation (1) above:
  • the admittance proportional to the pressure can be known; hence, a barometer detecting the pressure can be constituted.
  • FIG. 6 shows another embodiment of the present invention.
  • Reference numeral 7' is a resistor connected in series with the piezoelectric oscillator 6, and the current at resonance flowing through the piezoelectric oscillator generates a potential across the resistor 7' when it flows through said resistor.
  • Reference numeral 11 represents an amplifier which amplifies the terminal voltage of the resistor 7' to a necessary level. A part of the output voltage of the amplifier 11 is applied to the phase comparator 8 while another is applied to an amplifier 12. The terminal voltage of the resistor is further amplified by this amplifier 12 and deflects the pointer of the voltmeter 10.
  • the deflection angle of the pointer of the voltmeter is proportional to the current of the piezoelectric oscillator at resonance, the gas pressure around the piezoelectric oscillator can be known from the deflection angle of the pointer.
  • a d.c. voltmeter or a d.c. ammeter can of course be used economically if a rectification circuit is disposed inside the amplifier 12.
  • FIG. 7 shows another embodiment of the present invention.
  • reference numeral 5 represents a frequency control circuit such as a voltage control oscillator which is capable of changing said frequency.
  • the variable frequency range of this frequency control circuit 5 is wider than the shift of the resonant frequency within a pressure range to be measured by a piezoelectric oscillator 6.
  • the output from the frequency control circuit 5 is applied to the piezoelectric oscillator 6, and the output of this oscillator 6 is applied to a current-voltage converter 7.
  • the current-voltage converter 7 generates a voltage proportional to a current flowing through the piezoelectric oscillator 6.
  • phase characteristics of the a.c. resistance of the piezoelectric oscillator 6, that is, the impedance, is zero (degree) at the resonance frequency f o as shown in FIG. 7. Therefore, the phase characteristics of the output voltage of the frequency control circuit 5 are the same as those of the output voltage of the current-voltage converter 7 at the resonant frequency f o , but the output voltage of the current-voltage converter 7 having the same phase as the current flowing through the piezoelectric oscillator 6 lags behind the output voltage of the frequency control circuit 5 at a frequency lower than the resonant frequency.
  • a phase comparator 8 detects the phase difference between the output voltage of the frequency control circuit 5 and the output voltage of the current-voltage converter 7.
  • the phase comparator 8 generates a voltage proportional to the phase difference.
  • This output voltage is in turn applied to a frequency control terminal of the frequency control circuit 5, and a feedback loop is formed so that the frequency of the voltage applied to the piezoelectric oscillator 6 always coincides with the resonant frequency.
  • Reference numeral 9 represents a low-pass filter which is connected to the phase comparator 8. Normally, the low-pass filter 9 is disposed so as to eliminate the high frequency component (noise) of the output of the phase comparator 8 and to stabilize the system.
  • the a.c. voltage which is always applied to the piezoelectric oscillator and has a frequency equal to the resonant frequency and the output voltage of the current-voltage converter 7 are applied to an operational circuit 13, which calculates the final value of equation (1).
  • the output of this operational circuit is applied to a voltmeter 10, which displays an a.c. resistance value corresponding to the pressure.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Fluid Pressure (AREA)

Abstract

The present invention provides a barometer which includes a frequency control circuit connected to the input of the piezoelectric oscillator, a current-voltage converter connected to the output of the piezoelectric oscillator, a phase comparator connected to the output of the frequency control circuit and to the output of the current-voltage converter, a voltmeter connected to the current-voltage converter, a voltmeter connected to the phase comparator, a low-pass filter connected to the phase comparator, and input means for applying the output of the low-pass filter to the frequency control circuit. In the construction described above, the ambient pressure of the gas around the piezoelectric oscillator is represented by the a.c. voltage value of the piezoelectric oscillator.

Description

BACKGROUND OF THE INVENTION
This invention relates to a barometer utilizing a piezoelectric oscillator.
It is known that the a.c. voltage of a piezoelectric oscillator which is disposed inside a pressure vessel and causes bending oscillation at a series resonant frequency, changes with pressure as shown in FIG. 2. Therefore, if this a.c. resistance value is known, the pressure corresponding to the resistance value can be known.
Various methods of measuring the a.c. resistance value are known, and a typical example is shown in FIG. 3. An oscillator 1 generates an a.c. voltage es of a frequency f. Reference numerals 2 and 3 represent an element to be measured and an amplifier, respectively. They constitute a current-voltage converter together with a feedback resistor RF, and the output voltage of the converter is eo. The amplifier is selected so that a current ix, flowing through the element to be measured, and a current iF, flowing through the feedback resistor, are equal. According to this system, the a.c. resistance Zx of the element to be measured is determined by the equation (1):
Z.sub.x =R.sub.F (e.sub.s /e.sub.o)                        (1)
OBJECT OF THE INVENTION
However, when a piezoelectric oscillator is used as the sensor of a voltmeter in the prior art construction described above, the resonant frequency of the piezoelectric oscillator changes with pressure as shown in FIG. 4. If the system shown in FIG. 3, which is a typical conventional construction, is used, the frequency of the oscillator 1 must always search out the resonant frequency to effect measurement, and this is very troublesome and time-consuming.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a circuit block diagram showing a barometer in accordance with the present invention;
FIG. 2 is a diagram showing an a.c. resistance -v- pressure curve of an ordinary piezoelectric oscillator;
FIG. 3 is a circuit diagram showing a prior art current-voltage conversion circuit;
FIG. 4 is a diagram showing the pressure dependence of the resonant frequency of an ordinary piezoelectric oscillator;
FIG. 5 is a diagram showing the phase of the impedance of an ordinary piezoelectric oscillator; and
FIG. 6 is a circuit block diagram showing the barometer in accordance with another embodiment of the invention.
FIG. 7 is a circuit block diagram showing the barometer in accordance with another embodiment of the invention.
DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS OF THE INVENTION
Hereinafter, a preferred embodiment of the barometer of this invention will be described in detail with reference to the accompanying drawings.
FIG. 1 is a circuit diagram showing the barometer in accordance with the present invention. Reference numeral 5 represents a frequency control circuit such as a voltage control oscillator which is capable of changing said frequency. The variable frequency range of this frequency control circuit 5 is wider than the shift of the resonant frequency within the pressure range to be measured by the piezoelectric oscillator 6. The output from the frequency control circuit 5 is applied to the piezoelectric oscillator 6, and the output of this oscillator 6 is applied to a current-voltage converter 7. The current-voltage converter 7 generates a voltage proportional to a current flowing through the piezoelectric oscillator 6.
The phase characterstics of the a.c. resistance of the piezoelectric oscillator 6, that is, the impedance, is zero (degrees) at the resonant frequency fo as shown in FIG. 5. Therefore, the phase characteristics of the output voltage of the frequency control circuit 5 are the same as those of the output voltage of the current-voltage converter 7 at the resonant frequency fo, but the voltage of the current-voltage converter 7, having the same phase as the current flowing through the piezoelectric oscillator 6, lags behind the output voltage of the frequency control circuit 5 at frequencies lower than the resonant frequency.
Therefore, a phase comparator 8 detects the phase difference between the output voltage of the frequency control circuit 5 and the output voltage of the current-voltage converter 7. The phase comparator 8 generates a voltage proportional to the phase difference. This output voltage is in turn applied to a frequency control terminal of the frequency control circuit 5, and a feedback loop is formed so that the frequency of the voltage applied to the piezoelectric oscillator 6 always coincides with the resonant frequency. Reference numeral 9 represents a low-pass filter which is connected to the phase comparator 8. Normally, the low-pass filter 9 is disposed so as to eliminate the high frequency component (noise) of the output of the phase comparator 8 and to stabilize the system.
The output of the current-voltage converter 7 can be expressed by the following equation (2) from equation (1) above:
l.sub.o =l.sub.s ·R.sub.F /Z.sub.x                (2)
Since the circuit is constructed so that es is always constant and since RF is resistance, the product es ·RF is a constant (es ·RF =K), and lo is given by equation (3) with the reciprocal of the impedance Zx being the admittance Yx: 
l.sub.o =K·Y.sub.x                                (3)
If this output is applied to the voltmeter 10, the admittance proportional to the pressure can be known; hence, a barometer detecting the pressure can be constituted.
FIG. 6 shows another embodiment of the present invention. Reference numeral 7' is a resistor connected in series with the piezoelectric oscillator 6, and the current at resonance flowing through the piezoelectric oscillator generates a potential across the resistor 7' when it flows through said resistor. Reference numeral 11 represents an amplifier which amplifies the terminal voltage of the resistor 7' to a necessary level. A part of the output voltage of the amplifier 11 is applied to the phase comparator 8 while another is applied to an amplifier 12. The terminal voltage of the resistor is further amplified by this amplifier 12 and deflects the pointer of the voltmeter 10. Since the deflection angle of the pointer of the voltmeter is proportional to the current of the piezoelectric oscillator at resonance, the gas pressure around the piezoelectric oscillator can be known from the deflection angle of the pointer. Though not described in detail in this embodiment, a d.c. voltmeter or a d.c. ammeter can of course be used economically if a rectification circuit is disposed inside the amplifier 12.
FIG. 7 shows another embodiment of the present invention.
In FIG. 7, reference numeral 5 represents a frequency control circuit such as a voltage control oscillator which is capable of changing said frequency. The variable frequency range of this frequency control circuit 5 is wider than the shift of the resonant frequency within a pressure range to be measured by a piezoelectric oscillator 6. The output from the frequency control circuit 5 is applied to the piezoelectric oscillator 6, and the output of this oscillator 6 is applied to a current-voltage converter 7. The current-voltage converter 7 generates a voltage proportional to a current flowing through the piezoelectric oscillator 6.
The phase characteristics of the a.c. resistance of the piezoelectric oscillator 6, that is, the impedance, is zero (degree) at the resonance frequency fo as shown in FIG. 7. Therefore, the phase characteristics of the output voltage of the frequency control circuit 5 are the same as those of the output voltage of the current-voltage converter 7 at the resonant frequency fo, but the output voltage of the current-voltage converter 7 having the same phase as the current flowing through the piezoelectric oscillator 6 lags behind the output voltage of the frequency control circuit 5 at a frequency lower than the resonant frequency.
Therefore, a phase comparator 8 detects the phase difference between the output voltage of the frequency control circuit 5 and the output voltage of the current-voltage converter 7. The phase comparator 8 generates a voltage proportional to the phase difference. This output voltage is in turn applied to a frequency control terminal of the frequency control circuit 5, and a feedback loop is formed so that the frequency of the voltage applied to the piezoelectric oscillator 6 always coincides with the resonant frequency. Reference numeral 9 represents a low-pass filter which is connected to the phase comparator 8. Normally, the low-pass filter 9 is disposed so as to eliminate the high frequency component (noise) of the output of the phase comparator 8 and to stabilize the system.
The a.c. voltage which is always applied to the piezoelectric oscillator and has a frequency equal to the resonant frequency and the output voltage of the current-voltage converter 7 are applied to an operational circuit 13, which calculates the final value of equation (1). The output of this operational circuit is applied to a voltmeter 10, which displays an a.c. resistance value corresponding to the pressure.

Claims (3)

We claim:
1. In a barometer of the type which measures pressure from an a.c. resistance value of a piezoelectric oscillator disposed inside a pressure vessel, a barometer consisting essentially of:
a frequency control circuit connected to the input of said piezoelectric oscillator;
a current-voltage converter connected to the output of said piezoelectric oscillator;
a phase comparator connected to the output of said frequency control circuit and to the output of said current-voltage converter;
a voltmeter connected to said current-voltage converter;
a low-pass filter connected to said phase comparator; and
input means for applying the output of said low-pass filter to said frequency control circuit;
the a.c. voltage value of said piezoelectric oscillator indicating the ambient pressure of a gas around said piezoelectric oscillator.
2. The barometer as defined in claim 1 which further includes an amplifier detecting a current flowing through said piezoelectric oscillator at resonance by means of a terminal voltage of a resistor connected in series with said piezoelectric oscillator and amplifying the terminal voltage of said resistor, and in which the gas pressure around said piezoelectric oscillator is indicated by the output voltage of said amplifier.
3. The barometer as defined in claim 1 which further includes an operational circuit connected to the output of said frequency control circuit and to the output of said current-voltage converter, and said voltmeter connected to the output of said operational circuit.
US06/715,496 1984-03-26 1985-03-25 Barometer Expired - Fee Related US4597288A (en)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
JP5803284A JPS60201225A (en) 1984-03-26 1984-03-26 Gas manometer
JP59-58032 1984-03-26
JP13067684A JPS6110735A (en) 1984-06-25 1984-06-25 Gas pressure gage
JP59-130676 1984-06-25

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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5347870A (en) * 1992-01-29 1994-09-20 State University Of New York Dual function system having a piezoelectric element
EP0764842A2 (en) * 1995-09-20 1997-03-26 Axiom Co., Ltd. Frequency deviation detecting circuit and measuring apparatus using the frequency deviation detecting circuit
DE10018665A1 (en) * 2000-04-14 2001-10-25 Siemens Ag Length sensor as high pressure sensor for measuring very high pressures in diesel combustion engine fuel-injection system common-rail
DE10063535A1 (en) * 2000-12-20 2002-07-04 Deutsch Zentr Luft & Raumfahrt Measurement of one or more changing state values of an elastic system, e.g. a vibration component, using a electro-mechanical transducer where the transducer impedance is used as a measurement value
WO2005114125A3 (en) * 2004-05-13 2006-11-16 Trintec Ind Inc Electronic instrument movement/barometer
US20070197893A1 (en) * 2004-04-23 2007-08-23 Makoto Nakai Pressure Measuring Method, Pressure Measuring Device, And Tonometer

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0690101B2 (en) * 1986-03-28 1994-11-14 株式会社長野計器製作所 Gas pressure gauge

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3541849A (en) * 1968-05-08 1970-11-24 James P Corbett Oscillating crystal force transducer system
JPS57136131A (en) * 1981-02-17 1982-08-23 Sharp Corp Barometer
US4490606A (en) * 1982-04-26 1984-12-25 Geosource Inc. Transducer apparatus utilizing fiber optics for data transmission

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5838738B2 (en) * 1979-01-11 1983-08-25 横河電機株式会社 pressure gauge
DE2934093C2 (en) * 1979-08-23 1984-12-20 Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V., 8000 München Frequency analog sensor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3541849A (en) * 1968-05-08 1970-11-24 James P Corbett Oscillating crystal force transducer system
JPS57136131A (en) * 1981-02-17 1982-08-23 Sharp Corp Barometer
US4490606A (en) * 1982-04-26 1984-12-25 Geosource Inc. Transducer apparatus utilizing fiber optics for data transmission

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
Review of Scientific Instruments, vol. 33, No. 1, Jan. 1962, pp. 47 49. *
Review of Scientific Instruments, vol. 33, No. 1, Jan. 1962, pp. 47-49.

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5347870A (en) * 1992-01-29 1994-09-20 State University Of New York Dual function system having a piezoelectric element
EP0764842A2 (en) * 1995-09-20 1997-03-26 Axiom Co., Ltd. Frequency deviation detecting circuit and measuring apparatus using the frequency deviation detecting circuit
EP0764842A3 (en) * 1995-09-20 1998-08-19 Axiom Co., Ltd. Frequency deviation detecting circuit and measuring apparatus using the frequency deviation detecting circuit
DE10018665A1 (en) * 2000-04-14 2001-10-25 Siemens Ag Length sensor as high pressure sensor for measuring very high pressures in diesel combustion engine fuel-injection system common-rail
DE10018665B4 (en) * 2000-04-14 2006-12-14 First Sensor Technology Gmbh Length sensor with piezo effect
DE10063535A1 (en) * 2000-12-20 2002-07-04 Deutsch Zentr Luft & Raumfahrt Measurement of one or more changing state values of an elastic system, e.g. a vibration component, using a electro-mechanical transducer where the transducer impedance is used as a measurement value
DE10063535C2 (en) * 2000-12-20 2003-08-14 Deutsch Zentr Luft & Raumfahrt Procedure for the determination of variable state variables of an elastic system
CN100571610C (en) * 2004-04-23 2009-12-23 学校法人早稻田大学 Pressure measurement method, pressure gauge and tonometer
US20070197893A1 (en) * 2004-04-23 2007-08-23 Makoto Nakai Pressure Measuring Method, Pressure Measuring Device, And Tonometer
US7713197B2 (en) * 2004-04-23 2010-05-11 Waseda University Pressure measuring method, pressure measuring device, and tonometer
WO2005114125A3 (en) * 2004-05-13 2006-11-16 Trintec Ind Inc Electronic instrument movement/barometer
US7493813B2 (en) 2004-05-13 2009-02-24 Brendon G. Nunes Electronic instrument movement/barometer
US20080190196A1 (en) * 2004-05-13 2008-08-14 Nunes Brendon G Electronic Instrument Movement/Barometer

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Publication number Publication date
EP0157533A2 (en) 1985-10-09
DE3583055D1 (en) 1991-07-11
EP0157533A3 (en) 1989-05-10
EP0157533B1 (en) 1991-06-05

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